Geant4 10.7.0
Toolkit for the simulation of the passage of particles through matter
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G4FPYNormalFragmentDist.cc
Go to the documentation of this file.
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26/*
27 * File: G4FPYNormalFragmentDist.cc
28 * Author: B. Wendt ([email protected])
29 *
30 * Created on July 26, 2011, 12:26 PM
31 */
32
33#include "G4Ions.hh"
34#include "Randomize.hh"
35#include "globals.hh"
36
38#include "G4FFGEnumerations.hh"
41
43G4FPYNormalFragmentDist( G4int WhichIsotope,
44 G4FFGEnumerations::MetaState WhichMetaState,
46 G4FFGEnumerations::YieldType WhichYieldType,
47 std::istringstream& dataFile)
48: G4FissionProductYieldDist( WhichIsotope,
49 WhichMetaState,
50 WhichCause,
51 WhichYieldType,
52 dataFile)
53{
54 // Initialize the class
55 Initialize();
56}
57
59G4FPYNormalFragmentDist( G4int WhichIsotope,
60 G4FFGEnumerations::MetaState WhichMetaState,
62 G4FFGEnumerations::YieldType WhichYieldType,
63 G4int Verbosity,
64 std::istringstream& dataFile)
65: G4FissionProductYieldDist( WhichIsotope,
66 WhichMetaState,
67 WhichCause,
68 WhichYieldType,
69 Verbosity,
70 dataFile)
71{
72 // Initialize the class
73 Initialize();
74}
75
77Initialize( void )
78{
80
81 // Nothing here yet
82
84}
85
88{
90
91 G4Ions* Particle;
92
93 // Generate a (0, 1] random number and return the respective particle.
94 // The ENDF data tables lists 72172 as the largest fission fragment produced
95 // for any fission event. The maximum alpha production is 10 and the
96 // smallest fissile isotope is 90227. This means that if isotope 72172 were
97 // selected as the first daughter product, then at 10 alpha particles only
98 // 15 nucleons and -2 protons would remain for the second daughter product.
99 // Although the actual probability of this occurring is very small, or 0 in
100 // this case, a check should still be made to ensure that the second
101 // daughter product can be physically realized. This would prevent a
102 // situation such as this extreme example which results in a nucleus of 13
103 // neutrons and 2 anti-protons.
104 // This quick sanity check may become even more valid if the ENDF data
105 // tables are expanded in the future and include larger fission products.
106
107 G4int icounter=0;
108 G4int icounter_max=1024;
109 do
110 {
111 icounter++;
112 if ( icounter > icounter_max ) {
113 G4cout << "Loop-counter exceeded the threshold value at " << __LINE__ << "th line of " << __FILE__ << "." << G4endl;
114 break;
115 }
117 } while(Particle->GetAtomicMass() > RemainingA_ + 1
118 || Particle->GetAtomicNumber() > RemainingZ_ + 1);
119 // Loop checking, 11.05.2015, T. Koi
120
122 return Particle;
123}
124
126{
128
129 // Empty - all the data elements to be deconstructed are removed by
130 // ~G4FissionProductYieldDist()
131
133}
#define G4FFG_FUNCTIONLEAVE__
#define G4FFG_FUNCTIONENTER__
int G4int
Definition: G4Types.hh:85
#define G4endl
Definition: G4ios.hh:57
G4GLOB_DLL std::ostream G4cout
virtual G4Ions * GetFissionProduct(void)
G4FPYNormalFragmentDist(G4int WhichIsotope, G4FFGEnumerations::MetaState WhichMetaState, G4FFGEnumerations::FissionCause WhichCause, G4FFGEnumerations::YieldType WhichYieldType, std::istringstream &dataFile)
G4double G4SampleUniform(void)
G4Ions * FindParticle(G4double RandomParticle)
Definition: G4Ions.hh:52